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 /* NRDF D1797 Data No.1                                              */
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 /* Bibliography                                                      */
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 \\BIB,1;
 D#=D1797;
 TITLE=/Isobaric analog state of 14Be/;
 PURPOSE=/To measure the Isobaric Analog State (IAS) of the
          neutron-dripline nucleus 14Be for the first time in a
          charge-exchange reactino 14Be(p,n)14B* in inverse kinematics
          at E(14Be) = 74 AMeV./;
 ATH=(S.TAKEUCHI'1', S.SHIMOURA'2', T.MOTOBAYASHI'1', H.AKIYOSHI'3',
      Y.ANDO'1', N.AOI'4', ZS.FULOP'5', T.GOMI'1', Y.HIGURASHI'1',
      M.HIRAI'6', N.IWASA'7', H.IWASAKI'2', Y.IWATA'6',
      H.KOBAYASHI'1', M.KUROKAWA'2', Z.LIU'8', T.MINEMURA'3',
      S.OZAWA'3', H.SAKURAI'4', M.SERATA'1', T.TERANISHI'2',
      K.YAMADA'1', Y.YANAGISAWA'3', M.ISHIHARA'3');
 INST-ATH=(2JPNYOK'1', 2JPNTOK'2', 2JPNIPC'3', 2JPNTOK'4', 3HUNDEB'5',
           2JPNIRS'6', 2JPNTOH'7', 3CPRIMP'8');
      /* '1' Department of Physics */
      /* '2' Center for Nuclear Study (CNS) */
      /* '4' Department of Physics */
      /* '7' Department of Physics */
 REF=PL/B;
 VLP=515(2001)255;
 RCTS=(P(14BE,14B)N, D(14BE,14B)X);
 PHQS=(ENGY-SPEC, ANGL-DSTRN, X'9', X'10', COULOMB-DISP-ENGY'11');
 /* '9' Energy and width of the peak of the decay energy spectra of
    the 12Be + p + n channel for the (p,n) reaction */
 /* '10' Excitation energy of the IAS */
 /* '11' Coulomb displacement energy for the pair of 14Be and its
    IAS. */
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 /* Experimental Conditions                                           */
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 \\EXP,1;
 /* 2003-07-09 : Compiled */
 ENR=X%;
 PHYS-FORM=SLD;
 BAC=X;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=(CYC'12',PRJFS'13');
 /* '12' Primary beam of 100 AMeV 18O on a 1110 mg/cm**2 thic 9Be
        target */
 /* '13' Secondary beam of 14Be selected by the RIKEN Projectile
        Fragment Separator (RIPS) [T.Kubo et al., Nucl. Instrum. Methods
        B70(1992)309]. */
 INST-ACC=(2JPNIPC'12',2JPNIPC'13');
 INC-ENGY-LAB=74MEV/A;
 ERS-PRJ=8MEV/A;
 BEAM-INTNSTY=1e4PPS'14';
 /* '14' Typical intensity of the 14Be beam with a purity of
         around 80% */
 POL-PRJ=0%;
 DET-PARTCL=(P,N,12BE);
 COINC=(P,N,12BE);
 ANT-COINC=NO;
 DET-SYS=(PLST-SCT'15',TOF'16');
 /* '15' To detect decay particles from 14B*. Resolutions of TOF
         were about 1.2% (FWHM) for charged particles and about
         1.5%(FWHM) for neutrons at the energies of 74 AMeV. */
 /* '16' To determine velocities of the decay particles */
 ERS-DET=0.15MEV'17';
 /* '17' Resolution of decay energy at 0.3 MeV */
 /* Experimental Method:
    - Time-of-flight (To determine velocities of the decay particles)
 /* Analysis:
    - Invariant mass method
 RCT=P(14BE,14B)N;
 PHQ=ENGY-SPEC;
 CHM=CH2'18';
 /* '18' (CH2)n and C target are used, C target was used to
         subtract the contributions of carbon nuclei in the (CH2)n
         target. */
 THK-TGT=XMG/CM**2'19';
 /* '19' 187 and 152 mg/cm2 for (CH2)n and C target, respectively.
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 /* Descriptive Parameters                                            */
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 \\DATA,1;
 INC-ENGY-LAB=74MEV/A;
 SYS-ERR=10%'20';
 /* '20' Uncertainties for corrected and uncorrected spectra due
         to neutron detection efficiency and the reaction losses of the
         charged particles in hodoscope. */
 EMT-1=12BE;
 RSD=N;
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 /* Data Table                                                        */
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 \DATA;
 EXC-ENGY-EMT'21' DATA1'22' DSIGMA/DE DELTA-DSIGMA/DE'23'
 DATA2'24' DELTA-DATA2'24' FLAG'25'
 (MEV) (MEV) (MB/MEV) (MB/MEV) (MB/MEV) (MB/MEV) (NODIM)
 16.770 0.000  0.000 +-X      0.000 +-X       1
 16.845 0.075 -0.442 +-0.442 -0.023 +-0.023   2
 16.895 0.125  0.627 +-0.362  0.058 +-0.034   X
 16.945 0.175  0.432 +-0.350  0.056 +-0.045   X
 16.995 0.225  1.578 +-0.498  0.267 +-0.084   X
 17.045 0.275  2.208 +-0.522  0.459 +-0.109   X
 17.095 0.325  1.417 +-0.404  0.342 +-0.097   X
 17.170 0.400  0.862 +-0.208  0.238 +-0.057   X
 17.270 0.500  0.368 +-0.118  0.116 +-0.037   X
 17.370 0.600  0.276 +-0.099  0.096 +-0.034   X
 17.495 0.725  0.316 +-0.080  0.116 +-0.029   X
 17.645 0.875  0.273 +-0.079  0.102 +-0.030   X
 17.820 1.050  0.256 +-0.075  0.094 +-0.027   X
 18.020 1.250  0.244 +-0.077  0.084 +-0.027   X
 18.220 1.450  0.429 +-0.093  0.134 +-0.029   X
 18.445 1.675  0.474 +-0.107  0.127 +-0.029   X
 18.695 1.925  0.434 +-0.134  0.101 +-0.030   X
 18.970 2.200  0.611 +-0.141  0.114 +-0.026   X
 19.270 2.500  0.658 +-0.153  0.097 +-0.022   X
 19.595 2.825  0.847 +-0.179  0.097 +-0.021   X
 \END;
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